「
Since We Use Non-linear Artificial Diffusion
」を編集中
ナビゲーションに移動
検索に移動
警告:
ログインしていません。編集を行うと、あなたの IP アドレスが公開されます。
ログイン
または
アカウントを作成
すれば、あなたの編集はその利用者名とともに表示されるほか、その他の利点もあります。
スパム攻撃防止用のチェックです。 けっして、ここには、値の入力は
しない
でください!
<br>We carry out an unprecedented excessive-resolution simulation for the solar convection zone. Our calculation reproduces the quick equator and near-surface shear layer (NSSL) of differential rotation and electric [http://47.109.132.168:3000/aldadailey0098 Wood Ranger Power Shears shop] shears the near-floor poleward meridional movement concurrently. The NSSL is located in a posh layer where the spatial and time scales of thermal convection are significantly small in contrast with the deep convection zone. While there have been several attempts to reproduce the NSSL in numerical simulation, [https://gummipuppen-wiki.de/index.php?title=Regardless_Of_The_Brand_You_Choose Wood Ranger Power Shears] the results are nonetheless removed from reality. On this research, we reach reproducing an NSSL in our new calculation. 4) the turbulent viscosity and magnetic tension are latitudinally balanced with the Coriolis pressure in the NSSL. We emphasize the importance of the magnetic field in the photo voltaic convection zone. ††software: R2D2 Hotta et al. The Sun is rotating differentially with the quick equator and the slow pole. Omega within the photo voltaic interior. Within the solar convection zone, now we have two shear layers, i.e., the tachocline around the bottom of the convection zone and the near-floor shear layer (NSSL).<br><br><br><br>The tachocline is thought to be maintained by the interplay between the convection and radiation zones (Spiegel & Zahn, 1992; Gough & McIntyre, 1998; Forgács-Dajka & Petrovay, 2001; Rempel, 2005; Brun et al., 2011; Matilsky et al., 2022). The NSSL is thought to be maintained by the small-spatial and brief time scales of the convection within the layer. T/g, the place TT and gg are the temperature and the gravitational acceleration, [https://utshonews.com/?p=72 Wood Ranger Power Shears review] [http://60.247.149.237:3000/trenaupfield88 Wood Ranger Power Shears sale] [http://inprokorea.com/bbs/board.php?bo_table=free&wr_id=2181504 Wood Ranger Power Shears price] Shears order now respectively. 60 and a pair of Mm, respectively. Thus, the time scales of the convection vary from a month to several hours in these areas. Because of this, the convection within the NSSL isn't significantly affected by the rotation. ′ denote the longitudinal average and the deviation from the typical. As well as, Miesch & Hindman (2011) suggest that we'd like a [http://8.148.227.127:9980/susannahhorvat Wood Ranger Power Shears] to balance with the latitudinal Coriolis [http://wiki.konyvtar.veresegyhaz.hu/index.php?title=Answers_About_Flower_Gardening cordless power shears] to maintain the NSSL. It is troublesome for numerical simulations to cover a broad vary of spatial and time scales. The numerical approach for the NSSL is very restricted.<br> <br><br><br>Guerrero et al. (2013) enhance the superadiabaticity around the top boundary of their calculation field and focus on the formation mechanism of the NSSL following Foukal & Jokipii (1975). Hotta et al. NSSL-like feature, particularly at low and high latitudes. We argue there that the NSSL is maintained by the radially inward angular momentum transport and the turbulent viscosity on the sheared meridional circulation. Hotta et al. (2015) fail to reproduce the NSSL in mid-latitude. Matilsky et al. (2019) carry out an identical calculation to Hotta et al. 2015) and reproduce the NSSL-like feature at excessive and low latitudes. The authors also fail to reproduce the NSSL in the mid-latitude. They conclude that the detailed development mechanism of the meridional flow must be understood to reproduce the right NSSL. In their examine, highly rotationally constrained convection called the Busse column, is required to reproduce the photo voltaic-like quick equator differential rotation. Hotta et al. (2015) lowered the solar luminosity and Matilsky et al.<br><br><br><br>2019) elevated the rotation fee in order to boost the rotational affect on the thermal convection. We observe that the decrease in luminosity and the rise in rotation charge have the identical impact on the Rossby number. Matilsky et al. (2019) argue that when the rotationally constrained Busse column exists in the deep layer, upflows are rotationally constrained even within the near-floor high Rossby quantity layer. The efficient era of the close to-floor circulation by way of the gyroscopic pumping successfully suppresses the development of the NSSL. When the earlier calculation (Hotta et al., 2015; Matilsky et al., 2019) was carried out, we didn't have any way to maintain the photo voltaic-like DR without using the lowered luminosity, larger rotation charges or enhanced diffusivities (photo voltaic convective conundrum). That is, the typical "high-resolution" simulations fall into anti-photo voltaic differential rotation. O’Mara et al., 2016; Hotta et al., 2023). Hotta & Kusano (2021)(hereafter HK21) and Hotta et al. 2022)(hereafter HKS22) just lately present a attainable answer to construct the solar-like differential rotation with out utilizing particular treatment shown above.<br>
編集内容の要約:
鈴木広大への投稿はすべて、他の投稿者によって編集、変更、除去される場合があります。 自分が書いたものが他の人に容赦なく編集されるのを望まない場合は、ここに投稿しないでください。
また、投稿するのは、自分で書いたものか、パブリック ドメインまたはそれに類するフリーな資料からの複製であることを約束してください(詳細は
鈴木広大:著作権
を参照)。
著作権保護されている作品は、許諾なしに投稿しないでください!
編集を中止
編集の仕方
(新しいウィンドウで開きます)
案内メニュー
個人用ツール
ログインしていません
トーク
投稿記録
アカウント作成
ログイン
名前空間
ページ
議論
日本語
表示
閲覧
編集
履歴表示
その他
検索
案内
メインページ
最近の更新
おまかせ表示
MediaWikiについてのヘルプ
ツール
リンク元
関連ページの更新状況
特別ページ
ページ情報